Let . By the Tonelli theorem, is integrable on , since its integral is . The Plancherel theorem and periodization giveConsequently, if almost everywhere these inner products are , proving orthonormality. Conversely orthonormality says that every Fourier coefficient of is zero. The uniqueness of Fourier coefficients in L1 implies almost everywhere. HenceThis proves orthonormal translates and Fourier periodization, including both directions and the normalization constant associated with the printed Fourier transform.
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